
is in a cartesian basis

is in the crystal basis

is dimensionless, this is important, as in:

is the inverse

is the transpose

is the inverse transpose
To transform a vector of coordinates using M

To transform a tensor:

Then you apply your rotation:
 \mathrm{R}^t)
If you want go back into the crystal system:
 \mathrm{R}^t) \mathrm{M}^{-t})
After simplification:
 \beta_{\text{crys}} (\mathrm{M}^t \mathrm{R}^t \mathrm{M}^{-t}))
 \beta_{\text{crys}} (\mathrm{M}^{-1} \mathrm{R} \mathrm{M})^t)
I thought I explained this in a publication but not this case, not when the transformation is defined in a diferent basis.
http://scripts.iucr.org/cgi-bin/paper?S0108767311018216I forgot to mention that this is valid for beta but not for U as in the cif file. There are couple of steps more.